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Lecture 18 Selectivity Electrophysiology continued: V- gating The speed of spike propagation and the geometry of the axon Role of myelination

Lecture 18 Selectivity Electrophysiology continued: V-gating

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Lecture 18 Selectivity Electrophysiology continued: V-gating The speed of spike propagation and the geometry of the axon Role of myelination. Why are K+ channels highly selective for K+ and Na+ channels are not always highly selective for Na+? - PowerPoint PPT Presentation

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Page 1: Lecture 18 Selectivity Electrophysiology continued: V-gating

Lecture 18

Selectivity

Electrophysiology continued: V-gating

The speed of spike propagation and the geometry of the axon

Role of myelination

Page 2: Lecture 18 Selectivity Electrophysiology continued: V-gating

Why are K+ channels highly selective for K+ and Na+ channels are not always highly selective for Na+?

From the Goldman treatment we can see that a sufficient depolarization can be easily achieved with a non-selective cationic channel that passes both Na+ and K+. Indeed, we need to depolarize the membrane to the threshold (- 55 mV) to evoke excitation.

High selectivity for K+ is required specifically to re-polarize the cell to its resting state (-70 mV) and keep it there.

Page 3: Lecture 18 Selectivity Electrophysiology continued: V-gating

Potassium channel KcsA (from Streptomyces lividans)

carbonyl oxygens (red) substitute for water and provide high selectivity for potassium

Selectivity filter

Page 4: Lecture 18 Selectivity Electrophysiology continued: V-gating

In the selectivity filter of KcsA the K+ ion is overcoordinated relative to bulk water where only four molecules constitute the first hydration shell around the ion. It’s because water forms electrostatic H-bonds with the surrounding water which largely outcompete the ion. In contrast, there are no H-binding groups around the selectivity filter, which is dedicated to coordinate the ion only.

from Varma and Rempe, BJ 2007

Page 5: Lecture 18 Selectivity Electrophysiology continued: V-gating

from Varma and Rempe, BJ 2007

K+ ion can be coordinated by water (Hydroxyls), formamide (Carbonyls) and by di-glycine (Bidentate carbonyl ligands). The latter mimics the KcsA binding site and the computed free energy of transfer from water to this biding site is close to zero. This is the condition for the fastest transport in/out/across the channel.

Page 6: Lecture 18 Selectivity Electrophysiology continued: V-gating
Page 7: Lecture 18 Selectivity Electrophysiology continued: V-gating
Page 8: Lecture 18 Selectivity Electrophysiology continued: V-gating

Carbonyl oxygens cannot ‘come in touch’ with the smaller Na+ because they start repelling each other (partial charge ~-0.7e on each)

Page 9: Lecture 18 Selectivity Electrophysiology continued: V-gating

From Noskov, Berneshe and Roux, Nature,2004

According to Molecular Dynamics, the selectivity filter of KscA is not rigid, but can easily ‘collapse’ on a smaller Na+ ion. However, the resultant energy becomes higher due to repulsion between the carbonyl oxygens (see table on the next slide)

NMA = N-methylacetamide, a ligand that has carbonyls

Page 10: Lecture 18 Selectivity Electrophysiology continued: V-gating

From Noskov, Berneshe and Roux, Nature,2004

Page 11: Lecture 18 Selectivity Electrophysiology continued: V-gating

Selectivity Filter

Crowded with Charge

Wolfgang Nonner, Robert Eisenberg

+

++

The selectivity filter of L type Ca Channel consists of four Glutamic acid sidechains (EEEE) crowded in a narrow space. Ions are

attracted or excluded based on the charge/volume ratio

“E Side

Chains”

Page 12: Lecture 18 Selectivity Electrophysiology continued: V-gating

Selective Binding Curve: at approximately 10-6 M Ca2+ displaces Na+ in the selectivity filter L type Ca channel

Wolfgang Nonner

L type Ca Channel

Page 13: Lecture 18 Selectivity Electrophysiology continued: V-gating

13

Ion Diameters‘Pauling’ Diameters

Ca++ 1.98 Å

Na+ 2.00 Å

K+ 2.66 Å

‘Side Chain’ Diameter

Lysine K 3.00 Å

D or E 2.80 Å

Channel Diameter 6 Å

Parameters are Fixed in all calculations in all solutions for all mutants

Boda, Nonner, Valisko, Henderson, Eisenberg & Gillespie

‘Side Chains’ are Spheres Free to move inside channel

Snap Shots of Contents

In order to convert the channel from Ca to Na-selective, the EEEE motif can be changed to DEKA. All you need is to put the charges into a 6Ǻ confinement

Radial Crowding is Severe

Experiments and Calculations done at pH 8

Page 14: Lecture 18 Selectivity Electrophysiology continued: V-gating

The Voltage Sensor

++

+

electrometer

voltage-gated channel

kTzekTG

c

o eeP

P //

o

c

Charged transmembrane helix = voltage sensor

Voltage dependence of open probability

helices S1-S6

Page 15: Lecture 18 Selectivity Electrophysiology continued: V-gating

Upward motion of voltage-sensor helices (S4)

Page 16: Lecture 18 Selectivity Electrophysiology continued: V-gating

0 0.05 0.1 0.150

0.2

0.4

0.6

0.8

1

0

Po2 x( )

Po1 x( )

Po3 x( )

, V

kTzeGokTG

c

o eeP

P /)(/

oc PP 1

1

1

1 /)(/)(

/)(

kTzeGokTzeGo

kTzeGo

o ee

eP

10

4

2

310

/10381.1

106022.1

10

3

2

1

23

19

z

z

z

KT

KJk

Ce

kTG

Variations of the charge in the sensor change both the midpoint and the slope of activation curves

intrinsic bias

kTzeGo

o

o eP

P /)(

1

o

c

Page 17: Lecture 18 Selectivity Electrophysiology continued: V-gating

A semi-log plot provides limiting slope for Po at low potentials, which is proportional to z

, V

0 0.05 0.1 0.151 10 5

1 10 4

1 10 3

0.01

0.1

1

Po1 x( )

Po2 x( )

Po3 x( )

Page 18: Lecture 18 Selectivity Electrophysiology continued: V-gating

Typical z values for ion channels:

Shaker (delayed rectifier) z ~ 13 (3.25/subunit)

Various TRP channels z ~ 0.6-2

VDAC (mitochondrial anion channel) z~ 3-4

Page 19: Lecture 18 Selectivity Electrophysiology continued: V-gating

Scheme of VDAC gating under positive or negative membrane potentials

VDAC = voltage dependent anion channel, conducts ATP and ADP

positive ‘lip’

Page 20: Lecture 18 Selectivity Electrophysiology continued: V-gating

Modification of the gate by polyelectrolytes (dextran sulfate) dramatically changes apparent z in VDAC

Page 21: Lecture 18 Selectivity Electrophysiology continued: V-gating

Properties of different fibers (axons) in the peripheral NS

Fiber type Myelination Function Diameter Conduction velocity

μm m/s

A + motoneurons 12-20 70-120

A + Touch sensation 5-12 30-70

A + muscle spindle 3-6 15-30

A no pain, temperature 2-5 12-30

B + visceral afferents, 1-3 3-15auton. preganglion.

C no pain, temperature, 0.3-1.3 0.7-2.5auton. postganglion.

Page 22: Lecture 18 Selectivity Electrophysiology continued: V-gating

unmyelinated fiber myelinated fiber

=regular wire =High-frequency cable

What defines the speed of spike propagation?

Page 23: Lecture 18 Selectivity Electrophysiology continued: V-gating

-70

+30

Na+Na+

K+

K+

Page 24: Lecture 18 Selectivity Electrophysiology continued: V-gating

R

C

V1V2

Charging time: = RC(delay)

time

V1

V2

Page 25: Lecture 18 Selectivity Electrophysiology continued: V-gating

R

Cr

Delay =RC is proportional to 1/r, therefore velocity V ~ r

R = 1/G, therefore R ~ 1/r2

Internal conductance is proportional to the cross-section: G ~ r2

Capacitance is proportional to the surface area of the cylinder A ~ 2r L

therefore C ~ r

Na+

L

Page 26: Lecture 18 Selectivity Electrophysiology continued: V-gating

Invertebrates Vertebrates

0.8 mm in diameter

2-5 micrometers

Page 27: Lecture 18 Selectivity Electrophysiology continued: V-gating
Page 28: Lecture 18 Selectivity Electrophysiology continued: V-gating
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Page 30: Lecture 18 Selectivity Electrophysiology continued: V-gating
Page 31: Lecture 18 Selectivity Electrophysiology continued: V-gating

Po – intermembrane adhesion protein (immunoglobulin-like)PMP22 – helps compacting the membranesMBP – basic protein remaining in the cytosolGap junction proteins perforate membranes to allow nutrients

Page 32: Lecture 18 Selectivity Electrophysiology continued: V-gating

From

Hill

e, 2

00

1

Page 33: Lecture 18 Selectivity Electrophysiology continued: V-gating

Saltatory excitation in myelinated fibersFig. 8-17

Myelin coat reducesCAPACITANCE

Velocity is proportional to the internodal distance

Page 34: Lecture 18 Selectivity Electrophysiology continued: V-gating

Fig. 8-13